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Question: A parallel plate air capacitor has a capacitance \( 18\mu F \) . If the distance between the plates ...

A parallel plate air capacitor has a capacitance 18μF18\mu F . If the distance between the plates is trebled and a dielectric medium is introduced, the capacitance becomes 72μF72\mu F . The dielectric constant of the medium is
(A) 44
(B) 99
(C) 1212
(D) 22

Explanation

Solution

Hint
First calculate the electric field between the two plates. Using that, we can find the potential difference between them. From here we can find the capacitance of the system applying a suitable formula.
E=σε0\Rightarrow E = \dfrac{\sigma }{{{\varepsilon _0}}} where σ\sigma is the charge per unit area on the plates and ε0{\varepsilon _0} is the permittivity of free space.
Q=CV\Rightarrow Q = CV where QQ is the charge on the positive conductor and CC is called the capacitance.
σ=QA\Rightarrow \sigma = \dfrac{Q}{A} where AA is the area of the capacitor plate.

Complete step by step answer
A capacitor is a system of conductors and dielectric that can store electric charge. It consists of two conductors containing equal and opposite charges and has a potential difference VV between them.
The potential difference between the conductors is proportional to the charge on the capacitor and is given by the relation Q=CVQ = CV where QQ is the charge on the positive conductor and CC is called the capacitance.
Now, for a parallel plate air capacitor, the electric field between the plates is E=σε0E = \dfrac{\sigma }{{{\varepsilon _0}}} where σ\sigma is the charge per unit area on the plates and ε0{\varepsilon _0} is the permittivity of free space.
Now, we know that the potential difference between the two plates is given by, V=E×dV = E \times d where dd is the distance between the two plates.
Thus, substituting the value of VV in the equation Q=CVQ = CV , we get,
Q=CEd\Rightarrow Q = CEd
Putting E=σε0E = \dfrac{\sigma }{{{\varepsilon _0}}} and σ=QA\sigma = \dfrac{Q}{A} where AA is the area of the capacitor plate, we get
Q=C×QAε0×d\Rightarrow Q = C \times \dfrac{Q}{{A{\varepsilon _0}}} \times d
C=Aε0d\Rightarrow C = \dfrac{{A{\varepsilon _0}}}{d}
This value is given to be 18μF18\mu F .
Now, we are told that a dielectric medium of constant KK is introduced between the conducting plates and the separation is increased by three times. So substituting ε0{\varepsilon _0} with ε=Kε0\varepsilon = K{\varepsilon _0} and dd with 3d3d in the capacitance equation we get,
C=Aε3d\Rightarrow C = \dfrac{{A\varepsilon }}{{3d}}
C=A×Kε03d\Rightarrow C = \dfrac{{A \times K{\varepsilon _0}}}{{3d}}
72=K×183\Rightarrow 72 = \dfrac{{K \times 18}}{3}
Where this new capacitance is 72μF72\mu F
K=72×318=12\Rightarrow K = \dfrac{{72 \times 3}}{{18}} = 12
Therefore, the correct option is (C).

Note
To establish the capacitance of an isolated single conductor, we assume the conductor to be a part of a capacitor whose other conductor is at infinity. In this particular problem we deal with capacitance with uniform dielectric, but there are certain cases where a non-uniform dielectric is used which varies with distance. For such a case we take dKdx=α\dfrac{{dK}}{{dx}} = \alpha , where α\alpha is a constant.